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COMPARISON OF DIELECTRIC AND VISCOELASTIC RELAXATION BEHAVIOR OF POLYISOPRENE SOLUTIONS - COHERENCE IN SUBCHAIN MOTION

机译:聚异戊二烯溶液的介电和粘弹性松弛行为比较-子链运动的相干性

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Viscoelastic relaxation of polymer chains at long time scales is induced by their global motion. This motion also induces dielectric relaxation if the chains have dipoles parallel along their contour. However, the motion is differently reflected in the viscoelastic and dielectric quantities: The former reflects orientational anisotropy of stress-generating units in the chains (hereafter referred to as subchains) at respective times, while the latter reflects orientational correlation of the subchains at two separate times. Comparison of those two quantities enables us to specify details in the chain motion. In particular, for two extreme cases of incoherent and coherent subchain motion in each chain at short time scales, viscoelastic moduli G* are explicitly calculated from relaxation times tau p, and eigenfunctions f(p) for a local correlation function that represents the orientational correlation of the subchains. G(incoh)* and G(coh)* calculated for respective cases are quite different, and comparison with the G* data specifies the coherence of the subchain motion. On the basis of these backgrounds, G* were measured for solutions of a monodisperse cis-polyisoprene (PI-49; M = 48.8k) in oligobutadiene (OB-0.7, M = 0.7k) and compared with G(inEoh)* and G(coh)* (Dielectrically determined tau(p), and f(p) were available for the PI-49 solutions.) G(incoh) agreed with the G' data when the PI concentration c was less than the entanglement concentration c(e), but for c > c(e) significant deviation was observed. These results mean that the subchain motion is incoherent for nonentangled chains but some degree of coherence emerges for entangled chains. However, some incoherence still survived for the entangled chains even in a well-entangled state (M/M(e) congruent to 10), as evidenced from differences between the G' data and G(coh)' These findings were utilized to discuss the observed changes of the G* data with c and further to re-examine conventional interpretation for those changes in terms of the Zimm/Rouse/reptation dynamics. [References: 32]
机译:聚合物链的整体运动会引起聚合物链在长时间尺度上的粘弹性松弛。如果链的偶极子沿其轮廓平行,则此运动也会引起介电弛豫。但是,运动在粘弹性和介电量上有不同的反映:前者反映了各个时间链(以下称为子链)中应力产生单元的方向各向异性,而后者则反映了两个独立链中子链的方向相关性。次。这两个数量的比较使我们能够指定链运动中的细节。特别是,对于在短时间尺度上每条链中不连贯和连贯的子链运动的两种极端情况,从松弛时间tau p显式计算出粘弹性模量G *,并针对代表方向相关性的局部相关函数的本征函数f(p)子链。分别计算的G(incoh)*和G(coh)*完全不同,与G *数据进行比较可确定子链运动的相干性。根据这些背景,测量了单分散顺式聚异戊二烯(PI-49; M = 48.8k)在低聚丁二烯(OB-0.7,M = 0.7k)中的溶液的G *,并与G(inEoh)*和G(coh)*(PI-49溶液可使用电介质测定的tau(p)和f(p)。)当PI浓度c小于纠缠浓度c时,G(incoh)与G'数据一致。 (e),但对于c> c(e),观察到显着偏差。这些结果意味着,对于非纠缠链,子链运动是不连贯的,但是对于纠缠链,会出现一定程度的连贯性。但是,即使在纠缠状态下(M / M(e)等于10),纠缠链仍然存在一些不一致性,这从G'数据和G(coh)'之间的差异可以证明。用c观察到的G *数据的变化,并进一步从Zimm / Rouse / reptation动力学的角度重新检查这些变化的常规解释。 [参考:32]

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